\[ I_n = \int_{0}^{1} (1 - x^k)^n \cdot 1\, dx \] \[ I_n = (1 - x^k)^n \cdot x - nk \int_{0}^{1} (1 - x^k)^{n-1} \cdot x^{k-1}\, dx \] \[ I_n = nk \left[ \int_{0}^{1} \left( (1 - x^k)^n - (1 - x^k)^{n-1} \right) dx \right] \] \[ I_n = nk I_n - nk I_{n-1} \] \[ \frac{I_n}{I_{n-1}} = \frac{nk}{nk + 1} \] \[ \frac{I_{21}}{I_{20}} = \frac{21k}{1 + 21k} \] \[ = \frac{147}{148} \Rightarrow k = 7 \]
The given integral is:
\[ I_n = \int_0^1 (1 - x^k)^n dx. \]
Using integration by parts, we get:
\[ I_n = \frac{nk}{nk + 1} I_{n-1}. \]
Iterating this formula, the relationship becomes:
\[ \frac{I_n}{I_{n-1}} = \frac{nk}{nk + 1}. \]
Given:
\[ \frac{I_{21}}{I_{20}} = \frac{147}{148}, \]
we substitute into the formula:
\[ \frac{21k}{21k + 1} = \frac{147}{148}. \]
Cross-multiplying and solving:
\[ 148 \cdot 21k = 147 \cdot (21k + 1), \]
\[ 148 \cdot 21k = 147 \cdot 21k + 147, \]
\[ 21k = 147 \implies k = 7. \]
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
